{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:CKBLMCVXKM66KL5W26TXLV2LVB","short_pith_number":"pith:CKBLMCVX","canonical_record":{"source":{"id":"1611.06437","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2016-11-19T22:20:31Z","cross_cats_sorted":["cond-mat.stat-mech","quant-ph"],"title_canon_sha256":"fc598dd01c0547eb9dce08f9ba640f0ad544297426f098b95642aaa0fff55914","abstract_canon_sha256":"030fb67de49b2c962547702a660bd9d2d74b23d2b43e59bc79da5ab5735aaa0e"},"schema_version":"1.0"},"canonical_sha256":"1282b60ab7533de52fb6d7a775d74ba84fda1d4c76d537385d25528212d0f937","source":{"kind":"arxiv","id":"1611.06437","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.06437","created_at":"2026-05-18T00:48:43Z"},{"alias_kind":"arxiv_version","alias_value":"1611.06437v1","created_at":"2026-05-18T00:48:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.06437","created_at":"2026-05-18T00:48:43Z"},{"alias_kind":"pith_short_12","alias_value":"CKBLMCVXKM66","created_at":"2026-05-18T12:30:09Z"},{"alias_kind":"pith_short_16","alias_value":"CKBLMCVXKM66KL5W","created_at":"2026-05-18T12:30:09Z"},{"alias_kind":"pith_short_8","alias_value":"CKBLMCVX","created_at":"2026-05-18T12:30:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:CKBLMCVXKM66KL5W26TXLV2LVB","target":"record","payload":{"canonical_record":{"source":{"id":"1611.06437","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2016-11-19T22:20:31Z","cross_cats_sorted":["cond-mat.stat-mech","quant-ph"],"title_canon_sha256":"fc598dd01c0547eb9dce08f9ba640f0ad544297426f098b95642aaa0fff55914","abstract_canon_sha256":"030fb67de49b2c962547702a660bd9d2d74b23d2b43e59bc79da5ab5735aaa0e"},"schema_version":"1.0"},"canonical_sha256":"1282b60ab7533de52fb6d7a775d74ba84fda1d4c76d537385d25528212d0f937","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:48:43.879230Z","signature_b64":"2/oXfg/Kr//3bLwdnnIzsGZJfriBFFbn/5Z6XQBZQ8HUmBUjxjA++Y9grZ1toDlNMcApBG8lOqvp342Ce8I0Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1282b60ab7533de52fb6d7a775d74ba84fda1d4c76d537385d25528212d0f937","last_reissued_at":"2026-05-18T00:48:43.878764Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:48:43.878764Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1611.06437","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:48:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"91jPTSEiWLyi8W/H/71wPKY2kzFx7PMBHHkB4HcisNPCE6ioa1RSqq/V21HLnfqoP4cM4xvtxbnDv1/GzigUBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T15:38:10.755135Z"},"content_sha256":"831a188771362632997a63f9d0aea63c3198952b88403a383cc24f0349b7fc08","schema_version":"1.0","event_id":"sha256:831a188771362632997a63f9d0aea63c3198952b88403a383cc24f0349b7fc08"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:CKBLMCVXKM66KL5W26TXLV2LVB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fast forward to the classical adiabatic invariant","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","quant-ph"],"primary_cat":"physics.class-ph","authors_text":"Ayoti Patra, Christopher Jarzynski, Sebastian Deffner, Yi\\u{g}it Suba\\c{s}{\\i}","submitted_at":"2016-11-19T22:20:31Z","abstract_excerpt":"We show how the classical action, an adiabatic invariant, can be preserved under non-adiabatic conditions. Specifically, for a time-dependent Hamiltonian $H = p^2/2m + U(q,t)$ in one degree of freedom, and for an arbitrary choice of action $I_0$, we construct a \"fast-forward\" potential energy function $V_{\\rm FF}(q,t)$ that, when added to $H$, guides all trajectories with initial action $I_0$ to end with the same value of action. We use this result to construct a local dynamical invariant $J(q,p,t)$ whose value remains constant along these trajectories. We illustrate our results with numerical"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.06437","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:48:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PjDb1ue0vwh0m04BR9MEfF76+v4e9O3AfFDw0RdpyqgladDVOYl2uwmrQyo6aQwLBRr0HS0aZBwYA7Sd53dFCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T15:38:10.755906Z"},"content_sha256":"91ac984977eab4dfaf3dee627814d56bf409781d362e20d569353a6a02b8f1f3","schema_version":"1.0","event_id":"sha256:91ac984977eab4dfaf3dee627814d56bf409781d362e20d569353a6a02b8f1f3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CKBLMCVXKM66KL5W26TXLV2LVB/bundle.json","state_url":"https://pith.science/pith/CKBLMCVXKM66KL5W26TXLV2LVB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CKBLMCVXKM66KL5W26TXLV2LVB/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-10T15:38:10Z","links":{"resolver":"https://pith.science/pith/CKBLMCVXKM66KL5W26TXLV2LVB","bundle":"https://pith.science/pith/CKBLMCVXKM66KL5W26TXLV2LVB/bundle.json","state":"https://pith.science/pith/CKBLMCVXKM66KL5W26TXLV2LVB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CKBLMCVXKM66KL5W26TXLV2LVB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:CKBLMCVXKM66KL5W26TXLV2LVB","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"030fb67de49b2c962547702a660bd9d2d74b23d2b43e59bc79da5ab5735aaa0e","cross_cats_sorted":["cond-mat.stat-mech","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2016-11-19T22:20:31Z","title_canon_sha256":"fc598dd01c0547eb9dce08f9ba640f0ad544297426f098b95642aaa0fff55914"},"schema_version":"1.0","source":{"id":"1611.06437","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.06437","created_at":"2026-05-18T00:48:43Z"},{"alias_kind":"arxiv_version","alias_value":"1611.06437v1","created_at":"2026-05-18T00:48:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.06437","created_at":"2026-05-18T00:48:43Z"},{"alias_kind":"pith_short_12","alias_value":"CKBLMCVXKM66","created_at":"2026-05-18T12:30:09Z"},{"alias_kind":"pith_short_16","alias_value":"CKBLMCVXKM66KL5W","created_at":"2026-05-18T12:30:09Z"},{"alias_kind":"pith_short_8","alias_value":"CKBLMCVX","created_at":"2026-05-18T12:30:09Z"}],"graph_snapshots":[{"event_id":"sha256:91ac984977eab4dfaf3dee627814d56bf409781d362e20d569353a6a02b8f1f3","target":"graph","created_at":"2026-05-18T00:48:43Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We show how the classical action, an adiabatic invariant, can be preserved under non-adiabatic conditions. Specifically, for a time-dependent Hamiltonian $H = p^2/2m + U(q,t)$ in one degree of freedom, and for an arbitrary choice of action $I_0$, we construct a \"fast-forward\" potential energy function $V_{\\rm FF}(q,t)$ that, when added to $H$, guides all trajectories with initial action $I_0$ to end with the same value of action. We use this result to construct a local dynamical invariant $J(q,p,t)$ whose value remains constant along these trajectories. We illustrate our results with numerical","authors_text":"Ayoti Patra, Christopher Jarzynski, Sebastian Deffner, Yi\\u{g}it Suba\\c{s}{\\i}","cross_cats":["cond-mat.stat-mech","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2016-11-19T22:20:31Z","title":"Fast forward to the classical adiabatic invariant"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.06437","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:831a188771362632997a63f9d0aea63c3198952b88403a383cc24f0349b7fc08","target":"record","created_at":"2026-05-18T00:48:43Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"030fb67de49b2c962547702a660bd9d2d74b23d2b43e59bc79da5ab5735aaa0e","cross_cats_sorted":["cond-mat.stat-mech","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2016-11-19T22:20:31Z","title_canon_sha256":"fc598dd01c0547eb9dce08f9ba640f0ad544297426f098b95642aaa0fff55914"},"schema_version":"1.0","source":{"id":"1611.06437","kind":"arxiv","version":1}},"canonical_sha256":"1282b60ab7533de52fb6d7a775d74ba84fda1d4c76d537385d25528212d0f937","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1282b60ab7533de52fb6d7a775d74ba84fda1d4c76d537385d25528212d0f937","first_computed_at":"2026-05-18T00:48:43.878764Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:48:43.878764Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2/oXfg/Kr//3bLwdnnIzsGZJfriBFFbn/5Z6XQBZQ8HUmBUjxjA++Y9grZ1toDlNMcApBG8lOqvp342Ce8I0Cw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:48:43.879230Z","signed_message":"canonical_sha256_bytes"},"source_id":"1611.06437","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:831a188771362632997a63f9d0aea63c3198952b88403a383cc24f0349b7fc08","sha256:91ac984977eab4dfaf3dee627814d56bf409781d362e20d569353a6a02b8f1f3"],"state_sha256":"5f34e19b1089365e563cc805a2b42c367776937e349ed78b0d71373043eee16f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"peJGuGamowfnTgu+ssBmap0jqiDVzwzJb1UKcVCUbXVf+1q4UZ6n4ewdLw/GLjxd6Nw+lnXShkLmC8MLlZTOAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-10T15:38:10.760533Z","bundle_sha256":"f201d43a673165f4d2da44de9a8bd28454f72516f8774164440f3ebe476eec61"}}